EP0844465A1 - Method and system for spatial filtering of an extended radiation source with chromatic aberration of imaging optics in single-element detector measurement for monitoring of the extended radiation source - Google Patents
Method and system for spatial filtering of an extended radiation source with chromatic aberration of imaging optics in single-element detector measurement for monitoring of the extended radiation source Download PDFInfo
- Publication number
- EP0844465A1 EP0844465A1 EP96402542A EP96402542A EP0844465A1 EP 0844465 A1 EP0844465 A1 EP 0844465A1 EP 96402542 A EP96402542 A EP 96402542A EP 96402542 A EP96402542 A EP 96402542A EP 0844465 A1 EP0844465 A1 EP 0844465A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- radiation source
- wavelength
- extended radiation
- extended
- imaging optics
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 230000005855 radiation Effects 0.000 title claims abstract description 131
- 238000000034 method Methods 0.000 title claims abstract description 27
- 230000004075 alteration Effects 0.000 title claims abstract description 23
- 238000003384 imaging method Methods 0.000 title claims abstract description 22
- 238000012544 monitoring process Methods 0.000 title claims description 11
- 238000001914 filtration Methods 0.000 title claims description 9
- 238000005259 measurement Methods 0.000 title claims description 4
- 238000002834 transmittance Methods 0.000 claims abstract description 15
- 239000000835 fiber Substances 0.000 claims abstract description 13
- 238000012545 processing Methods 0.000 claims abstract description 9
- 230000007613 environmental effect Effects 0.000 claims abstract description 6
- 230000003595 spectral effect Effects 0.000 claims description 11
- 230000003252 repetitive effect Effects 0.000 claims description 5
- 238000010183 spectrum analysis Methods 0.000 claims description 4
- 230000005540 biological transmission Effects 0.000 claims description 2
- 238000001228 spectrum Methods 0.000 claims 2
- 230000001934 delay Effects 0.000 claims 1
- 230000000737 periodic effect Effects 0.000 claims 1
- 238000010586 diagram Methods 0.000 description 4
- 238000001514 detection method Methods 0.000 description 2
- 230000010354 integration Effects 0.000 description 2
- 230000033001 locomotion Effects 0.000 description 2
- 230000004048 modification Effects 0.000 description 2
- 238000012986 modification Methods 0.000 description 2
- 230000003287 optical effect Effects 0.000 description 2
- 230000003466 anti-cipated effect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000003913 materials processing Methods 0.000 description 1
Images
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J1/00—Photometry, e.g. photographic exposure meter
- G01J1/42—Photometry, e.g. photographic exposure meter using electric radiation detectors
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J1/00—Photometry, e.g. photographic exposure meter
- G01J1/02—Details
- G01J1/04—Optical or mechanical part supplementary adjustable parts
- G01J1/06—Restricting the angle of incident light
Definitions
- This invention relates to a method and system for monitoring the extended radiation source and, more particularly, to a method and system to apply the spatial filtering of an extended radiation source with chromatic aberration of imaging optics to the monitoring of the extended radiation source with single-element detector.
- the extended radiation source has been monitored for tracking, weld monitoring and autofocusing with single-element or array detectors.
- the array detector can monitor the variation of the extended radiation source easily, it cannot be used with a single-core fiber.
- the spatial filtering of an extended radiation source with chromatic aberration of imaging optics is applied to the monitoring of the variation of the extended radiation source.
- the local variation of an extended radiation source can be detected with single-element detectors, not with an array detector, for faster and easier monitoring the extended radiation source, and the remote operation with single core fiber transmission is possible.
- Fig. 1 of the drawings a schematic diagram of a simplified model for monitoring an extended radiation source is shown.
- the radiation from the extended radiation source 1 is collected and imaged on an aperture 3 by an imaging optics 2.
- the extended radiation source 1 can be either a self-radiating extended radiation source or an induced extended radiation source such as the weld pool generated by laser delivered through the same imaging optics 2.
- the imaging optics 2 consists of one or several lenses having large chromatic aberration.
- the aperture 3 can be either the detector itself or any physical aperture such as a hole or an input end of a fiber which delivers the laser to the imaging optics for laser materials processing.
- the only requirement for an aperture 3 is that all the radiation which passes the aperture 3 should be integrated by the detector 4.
- the spatial filtering is applied over the extended radiation source 1 for signal enhancement before the radiation gets to the detector 4 and is integrated over the extended radiation source 1. Due to the chromatic aberrations of imaging optics 2, the maximum effective radius of the extended radiation source which the detector 4 can see varies by the wavelengths.
- the " effective radius" means the radius where the transmittance times the intensity of radiation at that radius has some reasonable value for the contribution to the integrated signal.
- the transmittance of radiation from each element of the extended radiation source 1 to the detector 4 depends on the wavelengths of the radiation and the position of the radiation source element.
- the intensity profile of the radiation for each wavelength is multiplied by its own transmittance curve during the integration at detector 4.
- the shape of the intensity profile does not vary much by the wavelengths. In principle, it is quite similar to filtering process, and some wavelength having wider bandwidth can see the wider extended radiation source.
- the curves a, b are the transmittance curves for two wavelengths W a and W b
- the curves c, d are the intensity curves of the exteded radiation source at two moment, respectively. If the intensity curve of the extended radiation source is changed from curve c to curve d, the detector signal at wavelength W b can distinguish only the change in the intensity of the extended radiation source. However, in this case, the detector signal at wavelength W a can distinguish both the change in the size and the change in the intensity of the extended radiation source. Therefore, to remove the effect of the signal level change, the two signals are divided and the ratio of the detector signal at wavelength W a to that at wavelength W b can detect the change in the size of the extended radiation source without any interference from the change in the intensity of the extended radiation source.
- the factor which causes the variation of the transmittance curve can be detected and controlled.
- the transmittance curve depends also on the focus shift of the extended radiation source. Therefore, according to this invention, the focus informations can be obtained by processing the spatially-filtered multi-wavelength detector signals, and the focus of the extended radiation source can be controlled on the basis of the focus informations.
- a remote optical system for monitoring an extended radiation source 9 is shown.
- the radiation from the extended radiation source 9 is collected and imaged on the input end of a fiber 12 by an imaging optics 10.
- the imaging optics 10 consists of one or several lenses. If the spherical aberration of the imaging optics 10 becomes large compared to the chromatic aberration, the image blurring due to the spherical aberration reduces the chromatic discrimination by the wavelengths. Therefore, the lenses of the imaging optics 10 have high index of refraction to increase the chromatic aberration and to decrease the spherical aberration.
- the imaging optics 10 consists of two high index of refraction plano convex lenses 11a and 11b to reduce the image blurring due to the spherical aberration of the imaging optics.
- a fiber 12 is used as an aperture and also as means for the flexible delivery of radiation.
- the radiation of the extended radiation source 9 is imaged on the input end of the fiber 12 by the imaging optics 10, and delivered by the fiber 12.
- a collimating lens 13 is provided on front of the output end of the fiber 12.
- the radiation delivered through the fiber 12 is collimated by the collimating lens 13.
- dichromatic filters 14, 15 are provided after the collimating lens 13.
- wavelengths W 1 , W 2 , and W 3 are chosen in the order of W 1 ⁇ W 2 ⁇ W 3 for the spectral analysis of the extended radiation source.
- the wavelength W 2 is the wavelength to control the focus of the extended radiation source or the wavelength quite near to that control wavelength with almost same chromatic aberration.
- the wavelengths W 1 and W 3 are located further from the control wavelength and have much chromatic aberration with respect to the wavelength W 2 .
- a first dichromatic filter 14 and a second dichromatic filter 15 are used to split the radiation by wavelengths W 1 , W 2 , and W 3 .
- the number of dichromatic filter depends on the number of the subject wavelengths for the spectral analysis of the extended radiation source.
- the collimated radiation enters into the first dichromatic filter 14.
- the first dichromatic filter 14 transmits the radiation at wavelength W 1 but reflects at both wavelength W 2 and W 3 .
- the reflected radiation enters into the second dichromatic filter 15, which reflects the radiation at wavelength W 2 but transmits the radiation at wavelength W 3 .
- the splitted radiations pass the band-pass filters 16, 17 and 18.
- the band-pass filter 16 has only wavelength W 1 passed
- the band-pass filter 17 has only wavelength W 2 passed
- the band-pass filter 18 has only wavelength W 3 passed.
- the splitted and filtered radiations are collected on the corresponding detectors 22, 23, 24 by focusing lenses 19, 20, 21, respectively.
- the detectors 22, 23, 24 make the detector signals corresponding to wavelengths W 1 , W 2 , and W 3 .
- the detector signals from the detectors 22, 23, 24 are input to a computer 26 for signal processing by an interface 25.
- the diameter of the circular extended radiation source 9 is assumed to be near 1 mm and imaged by two SF6 lenses with 25 mm focal length and 8 mm clear aperture on the 1 mm core diameter fiber 12 with one to one magnification.
- Three wavelengths of 0.532 ⁇ m (wavelength W 1 ), 0.95 ⁇ m (wavelength W 2 ), and 1.5 ⁇ m (wavelength W 3 ) are chosen for spectral analysis.
- the dependence of the transmittance for each source element on the position of the source element over the extended radiation source and the focus shift of the extended radiation source can be calculated at three wavelengths with an optical analysis program. Owing to the circular symmetry, the radius of the source element is varied during the analysis.
- the transmittance curves vs. the radius of source element and the focus shift of the extended radiation source are shown in three-dimensional diagram in Figs. 4, 5, 6 and the data are listed in Figs. 7, 8, 9. In Figs. 4, 5, 6, x-direction represents the focus shift of the extended radiation source.
- the positive direction means the outward defocus region and the negative direction means the inward defocus region.
- the ratios of the two spectral signals, wavelength W 1 (0.532 ⁇ m) signal over wavelength W 2 (0.95 ⁇ m) signal or wavelength W 3 (1.5 ⁇ m) signal over wavelength W 2 (0.95 ⁇ m) signal can detect the change in the size of the extended radiation source between the two effective radii in outward or in inward defocus region respectively. Furthermore, the decrease of the effective radius with focus shift is noticeable at wavelength W 2 compared to the small decrease in the effective radius with focus shift at wavelength W 1 in the outward defocus region and that at wavelength W 3 in the inward defocus region.
- the signal at wavelength W 2 does not change since the change of the intensity occurs outside of the effective diameter at wavelength W 2 .
- the signals at wavelengths W 1 and W 3 in the outward defocus region and in the inward defocus region respectively corresponding to the variation of the intensity can be applied to detect the intensity change outside of the effective diameter at wavelength W 2 if the size of the extended radiation source is fixed.
- the signal at wavelength W 2 is very sensitive to the radial misalignment of the extended radiation source from the imaging optics axis compared to the signals at wavelength W 1 or W 3 . Therefore, instead of using the signal at wavelength W 2 for tracking of the extended radiation source, the ratio of the signal at wavelength W 1 over the signal at wavelength W 2 or the ratio of the signal at wavelength W 3 over the signal at wavelength W 2 can be used in the tracking of the extended radiation source where the intensity variation of the extended radiation source due to the environmental effects can be compensated by the division of the signals.
- the ratio of X/Y at the start of each repetitive process can detect the variation at the start of each process.
- the ratio of (X- X')/(Y-Y') where X' and Y' are measured with short time delay compared to the period of the repetitive process after the measurement of X and Y can detect the variation occurred after the start of each process, which possibly occurred due to the environmental effects.
- the environmental effects on the extended radiation source can be detected from the ratio of (X-X')/(Y-Y').
- the present invention can perform spatial filtering on the extended radiation source by which the local variation of the extended radiation source can be detected from the one-element detector signal.
- the present invention can detect the change thereof and control the extended radiation source, and in particular, the present invention can detect the local variation of the extended radiation source in realtime and repetitively.
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
Description
Claims (13)
- A method for detecting the local variation of extended radiation source from the single-element detector signals integrated over the extended radiation source comprising the steps of:focusing the radiation from an extended radiation source on an aperture with the imaging optics with chromatic aberration;transmitting the focused radiation from the extended radiation source througth an aperture;splitting the transmitted radiation by wavelength;focusing the splitted radiation on the detectors;detecting each wavelength signal integrated over the extended radiation source repetitively; andprocessing said signals to detect the local variation of the radiation intensity profile over the extended radiation source.
- A method as claimed in claim 1, further comprising the step of applying the spatial filtering to the chromatic intensity profile of the extended radiation source with a spatial filter for the signal processing to detect the local variation of the extended radiation source.
- A method as claimed in claim 2, further comprising the step of varing the bandwidth of the spatial filter for each chromatic intensity profile of the extended radiation source with the chromatic aberration of the imaging optics such that the effective size of the extended radiation source for the contribution to the integrated spectral signal varies by the wavelengths.
- A method as claimed in claim 3, wherein the spatial filter for each chromatic intensity profile is determined as the transmittance of that wavelength from each source element over the extended radiation source through the imaging optics and the aperture.
- A method as claimed in claim 1, further comprising the step of selecting the three wavelengths for the spectral analysis of the extended radiation source where the second wavelength is the wavelength to control the focus of the extended radiation source or the wavelength quite near to that control wavelength with almost same chromatic aberration, and the first wavelength is shorter than the second wavelength, and the third wavelength is longer than the second wavelength, and both the first and the third wavelength are located further from the control wavelength and have much chromatic aberration with respect to the second wavelength.
- A method as claimed in claim 1, wherein the variation of the size of the extended radiation source between the effective diameters of the measured wavelengths can be monitored from the spatially filtered spectral signals.
- A method as claimed in claim 1, wherein the signal processing of computing the ratio of the spatially filtered spectral signals is used in the control of the focus shift or the centering of the extended radiation source.
- A method as claimed in claim 1, wherein the signal processing of computing the ratio of the differences of spatially filtered spectral signals where the difference of each spatially filtered spectral signal is computed from the two measurements of that spectral signal measured with some delay is used to monitor the change of the extended radiation source including the change induced by environmental effects.
- A method as claimed in claims 7 and 8, wherein the signal processing of thd spectral signals is computed repetitively for the monitoring of the extended radiation source induced by the periodic process.
- A system for detecting the local variation of the extended radiation source comprising :imaging optics for the collection of the radiation from an extended radiation source with large chromatic aberration;an aperture to limit the transmission of the image of the extended radiation source;means for splitting and separating the spectrum of the radiation by wavelengths;an interface to digitize the spectral signals several times for each repetitive process with varying delays to detect the variation in each repetitive process and to monitor the change in time in each process; anda personal computer to process the spectral signals.
- A system as claimed in claim 10, wherein means for splitting and separating the spectrum of the radiation comprises :a collimating lens to collimate the diverging radiation out of the aperture;dichromatic filters to split the radiation by wavelengths;band-pass filters to narrow the bandwidth of each wavelength; andfocusing lenses to focus each chromatic radiation on the corresponding detector.
- A system as claimed in claim 10, wherein the aperture is replaced with a fiber for remote operation.
- A system as claimed in claim 10, wherein the imaging optic comprises one or several high index of refraction lenses.
Priority Applications (4)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE1996625489 DE69625489T2 (en) | 1996-11-26 | 1996-11-26 | Method and device for monitoring an extensive radiation source with single element detector measurement by means of spatial filtering and using the chromatic aberration of the imaging optics |
EP96402542A EP0844465B1 (en) | 1996-11-26 | 1996-11-26 | Method and system for spatial filtering of an extended radiation source with chromatic aberration of imaging optics in single-element detector measurement for monitoring of the extended radiation source |
AT96402542T ATE230105T1 (en) | 1996-11-26 | 1996-11-26 | METHOD AND DEVICE FOR MONITORING AN EXTENDED RADIATION SOURCE WITH SINGLE ELEMENT DETECTOR MEASUREMENT USING SPATIAL FILTERING AND USING THE CHROMATIC ABERRATION OF THE IMAGING OPTICS |
US08/763,752 US5875026A (en) | 1996-11-26 | 1996-12-11 | Method and system for spatial filtering of an extended radiation source with chromatic aberration of imaging optics in single-element detector measurement for monitoring of the extended radiation source |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP96402542A EP0844465B1 (en) | 1996-11-26 | 1996-11-26 | Method and system for spatial filtering of an extended radiation source with chromatic aberration of imaging optics in single-element detector measurement for monitoring of the extended radiation source |
US08/763,752 US5875026A (en) | 1996-11-26 | 1996-12-11 | Method and system for spatial filtering of an extended radiation source with chromatic aberration of imaging optics in single-element detector measurement for monitoring of the extended radiation source |
Publications (2)
Publication Number | Publication Date |
---|---|
EP0844465A1 true EP0844465A1 (en) | 1998-05-27 |
EP0844465B1 EP0844465B1 (en) | 2002-12-18 |
Family
ID=26144090
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP96402542A Expired - Lifetime EP0844465B1 (en) | 1996-11-26 | 1996-11-26 | Method and system for spatial filtering of an extended radiation source with chromatic aberration of imaging optics in single-element detector measurement for monitoring of the extended radiation source |
Country Status (2)
Country | Link |
---|---|
US (1) | US5875026A (en) |
EP (1) | EP0844465B1 (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6707550B1 (en) | 2000-04-18 | 2004-03-16 | Pts Corporation | Wavelength monitor for WDM systems |
Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3582666A (en) * | 1968-10-18 | 1971-06-01 | Erico Prod Inc | Light beam alignment and photoelectric receiver apparatus |
US4742222A (en) * | 1984-07-23 | 1988-05-03 | Tavkozlesi Kutato Intezet | Selective optical detector apparatus utilizing longitudinal chromatic aberration |
US4992859A (en) | 1988-03-29 | 1991-02-12 | Sony Corporation | Automatic focus control apparatus using primary color signals |
US5155329A (en) | 1990-01-08 | 1992-10-13 | Mitsubishi Jukogyo Kabushiki Kaisha | Monitoring method and system for laser beam welding |
WO1994015184A1 (en) * | 1992-12-28 | 1994-07-07 | Michele Hinnrichs | Image multispectral sensing |
US5444236A (en) | 1994-03-09 | 1995-08-22 | Loral Infrared & Imaging Systems, Inc. | Multicolor radiation detector method and apparatus |
Family Cites Families (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5206502A (en) * | 1976-10-21 | 1993-04-27 | The United States Of America As Represented By The Secretary Of The Navy | Laser radiation detection system |
US4909633A (en) * | 1986-05-12 | 1990-03-20 | Minolta Camera Kabushiki Kaisha | Multi-channel spectral light measuring device |
US5278402A (en) * | 1993-06-09 | 1994-01-11 | Litton Systems | Real-scene dispersion sensor detecting two wavelengths and determining time delay |
US5592285A (en) * | 1995-12-12 | 1997-01-07 | Pund; Marvin L. | Optical source position and direction sensor |
-
1996
- 1996-11-26 EP EP96402542A patent/EP0844465B1/en not_active Expired - Lifetime
- 1996-12-11 US US08/763,752 patent/US5875026A/en not_active Expired - Fee Related
Patent Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3582666A (en) * | 1968-10-18 | 1971-06-01 | Erico Prod Inc | Light beam alignment and photoelectric receiver apparatus |
US4742222A (en) * | 1984-07-23 | 1988-05-03 | Tavkozlesi Kutato Intezet | Selective optical detector apparatus utilizing longitudinal chromatic aberration |
US4992859A (en) | 1988-03-29 | 1991-02-12 | Sony Corporation | Automatic focus control apparatus using primary color signals |
US5155329A (en) | 1990-01-08 | 1992-10-13 | Mitsubishi Jukogyo Kabushiki Kaisha | Monitoring method and system for laser beam welding |
WO1994015184A1 (en) * | 1992-12-28 | 1994-07-07 | Michele Hinnrichs | Image multispectral sensing |
US5444236A (en) | 1994-03-09 | 1995-08-22 | Loral Infrared & Imaging Systems, Inc. | Multicolor radiation detector method and apparatus |
Also Published As
Publication number | Publication date |
---|---|
EP0844465B1 (en) | 2002-12-18 |
US5875026A (en) | 1999-02-23 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
EP0028774B1 (en) | Apparatus for detecting defects in a periodic pattern | |
US5076692A (en) | Particle detection on a patterned or bare wafer surface | |
US5623342A (en) | Raman microscope | |
EP1520173B1 (en) | Optical projection tomography | |
US8569680B2 (en) | Hyperacuity from pre-blurred sampling of a multi-aperture visual sensor | |
KR20060009308A (en) | Scanning laser microscope with wavefront sensor | |
CN103261857A (en) | Device and method for observing and for measuring Raman scattering | |
JPH01308930A (en) | Microspectroscopic apparatus | |
KR100443152B1 (en) | Method for monitoring the size variation and the focus shift of a weld pool in laser welding | |
EP1618423B1 (en) | Method of producing a compact wide-field-of-view imaging optical system | |
US4935630A (en) | Lens-sphere optical sensing system | |
CN110836642A (en) | Color triangular displacement sensor based on triangulation method and measuring method thereof | |
CN212988292U (en) | Piston rod surface roughness detecting system | |
EP0844465B1 (en) | Method and system for spatial filtering of an extended radiation source with chromatic aberration of imaging optics in single-element detector measurement for monitoring of the extended radiation source | |
FR2707018A1 (en) | ||
EP1160549A2 (en) | Sun optical limitation illumination detector | |
JPH0364816B2 (en) | ||
JP2000121499A (en) | Method and apparatus for measuring internal refractive index distribution of optical fiber base material | |
EP1136799B1 (en) | Method for processing low coherence interferometric data | |
KR102163216B1 (en) | Optical detecting device and control method the same | |
KR100193276B1 (en) | Monitoring method and device of light source using chromatic aberration and spatial filtration method of image optical system | |
JP2000509825A (en) | Optical scanning device | |
US7046354B2 (en) | Surface foreign matter inspecting device | |
JPH02304332A (en) | Particle measuring instrument | |
RU2397457C1 (en) | Displaying focal spectrometre (versions) |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
Free format text: ORIGINAL CODE: 0009012 |
|
17P | Request for examination filed |
Effective date: 19961130 |
|
AK | Designated contracting states |
Kind code of ref document: A1 Designated state(s): AT BE CH DE DK ES FI FR GB GR IE IT LI LU MC NL PT SE |
|
AKX | Designation fees paid |
Free format text: AT BE CH DE DK ES FI FR GB GR IE IT LI LU MC NL PT SE |
|
RBV | Designated contracting states (corrected) |
Designated state(s): AT BE CH DE DK ES FI FR GB GR IE IT LI LU MC NL PT SE |
|
GRAG | Despatch of communication of intention to grant |
Free format text: ORIGINAL CODE: EPIDOS AGRA |
|
17Q | First examination report despatched |
Effective date: 20020502 |
|
RAP1 | Party data changed (applicant data changed or rights of an application transferred) |
Owner name: KOREA ATOMIC ENERGY RESEARCH INSTITUTE |
|
GRAG | Despatch of communication of intention to grant |
Free format text: ORIGINAL CODE: EPIDOS AGRA |
|
GRAH | Despatch of communication of intention to grant a patent |
Free format text: ORIGINAL CODE: EPIDOS IGRA |
|
GRAH | Despatch of communication of intention to grant a patent |
Free format text: ORIGINAL CODE: EPIDOS IGRA |
|
GRAA | (expected) grant |
Free format text: ORIGINAL CODE: 0009210 |
|
AK | Designated contracting states |
Kind code of ref document: B1 Designated state(s): AT BE CH DE DK ES FI FR GB GR IE IT LI LU MC NL PT SE |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: NL Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20021218 Ref country code: LI Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20021218 Ref country code: IT Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRE;WARNING: LAPSES OF ITALIAN PATENTS WITH EFFECTIVE DATE BEFORE 2007 MAY HAVE OCCURRED AT ANY TIME BEFORE 2007. THE CORRECT EFFECTIVE DATE MAY BE DIFFERENT FROM THE ONE RECORDED.SCRIBED TIME-LIMIT Effective date: 20021218 Ref country code: GR Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20021218 Ref country code: FI Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20021218 Ref country code: CH Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20021218 Ref country code: BE Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20021218 Ref country code: AT Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20021218 |
|
REF | Corresponds to: |
Ref document number: 230105 Country of ref document: AT Date of ref document: 20030115 Kind code of ref document: T |
|
REG | Reference to a national code |
Ref country code: GB Ref legal event code: FG4D |
|
REG | Reference to a national code |
Ref country code: CH Ref legal event code: EP |
|
REG | Reference to a national code |
Ref country code: IE Ref legal event code: FG4D |
|
REF | Corresponds to: |
Ref document number: 69625489 Country of ref document: DE Date of ref document: 20030130 Kind code of ref document: P Ref document number: 69625489 Country of ref document: DE Date of ref document: 20030130 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: SE Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20030318 Ref country code: PT Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20030318 Ref country code: DK Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20030318 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: ES Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20030627 |
|
REG | Reference to a national code |
Ref country code: CH Ref legal event code: PL |
|
ET | Fr: translation filed | ||
PLBE | No opposition filed within time limit |
Free format text: ORIGINAL CODE: 0009261 |
|
STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: NO OPPOSITION FILED WITHIN TIME LIMIT |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: LU Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES Effective date: 20031126 Ref country code: IE Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES Effective date: 20031126 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: MC Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES Effective date: 20031130 |
|
26N | No opposition filed |
Effective date: 20030919 |
|
REG | Reference to a national code |
Ref country code: IE Ref legal event code: MM4A |
|
PGFP | Annual fee paid to national office [announced via postgrant information from national office to epo] |
Ref country code: DE Payment date: 20071108 Year of fee payment: 12 |
|
PGFP | Annual fee paid to national office [announced via postgrant information from national office to epo] |
Ref country code: FR Payment date: 20070928 Year of fee payment: 12 |
|
PGFP | Annual fee paid to national office [announced via postgrant information from national office to epo] |
Ref country code: GB Payment date: 20081107 Year of fee payment: 13 |
|
REG | Reference to a national code |
Ref country code: FR Ref legal event code: ST Effective date: 20090731 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: DE Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES Effective date: 20090603 |
|
GBPC | Gb: european patent ceased through non-payment of renewal fee |
Effective date: 20091126 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: GB Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES Effective date: 20091126 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: FR Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES Effective date: 20081130 |